<p>A bounded linear operator <i>A</i> on a complex Hilbert space <i>H</i> is a <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="44146_2025_208_Article_IEq1.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\rho \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ρ</mi> </math></EquationSource> </InlineEquation>-contraction (<InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="44146_2025_208_Article_IEq7.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\(\rho &gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ρ</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>) if there is a unitary operator <i>U</i> on space <i>K</i> containing <i>H</i> such that <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="44146_2025_208_Article_IEq8.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="117" /> </InlineMediaObject> <EquationSource Format="TEX">\(A^n=\rho P_HU^n|H\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>A</mi> <mi>n</mi> </msup> <mo>=</mo> <mi>ρ</mi> <msub> <mi>P</mi> <mi>H</mi> </msub> <msup> <mi>U</mi> <mi>n</mi> </msup> <mrow> <mo stretchy="false">|</mo> <mi>H</mi> </mrow> </mrow> </math></EquationSource> </InlineEquation> for all <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="44146_2025_208_Article_IEq9.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(n\ge 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>≥</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="44146_2025_208_Article_IEq10.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="24" /> </InlineMediaObject> <EquationSource Format="TEX">\(P_H\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>P</mi> <mi>H</mi> </msub> </math></EquationSource> </InlineEquation> denotes the orthogonal projection from <i>K</i> onto <i>H</i>. <i>U</i> is called a unitary <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="44146_2025_208_Article_IEq1.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\rho \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ρ</mi> </math></EquationSource> </InlineEquation>-dilation of <i>A</i>. Such operators originate from the early work of Sz.-Nagy and Foiaş (1966) and generalize the usual contractions and numerical contractions. In this survey, we briefly describe their properties, covering (1) their characterizations, (2) the related <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="44146_2025_208_Article_IEq1.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\rho \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ρ</mi> </math></EquationSource> </InlineEquation>-radius, defined as <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="44146_2025_208_Article_IEq13.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="203" /> </InlineMediaObject> <EquationSource Format="TEX">\(w_{\rho }(A)=\inf \{\lambda &gt;0 : (1/\lambda )A\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>w</mi> <mi>ρ</mi> </msub> <mrow> <mrow> <mo stretchy="false">(</mo> <mi>A</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mo movablelimits="true">inf</mo> <mo stretchy="false">{</mo> <mi>λ</mi> <mo>&gt;</mo> <mn>0</mn> <mo>:</mo> <mrow> <mo stretchy="false">(</mo> <mn>1</mn> <mo stretchy="false">/</mo> <mi>λ</mi> <mo stretchy="false">)</mo> </mrow> <mi>A</mi> </mrow> </mrow> </math></EquationSource> </InlineEquation> is a <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="44146_2025_208_Article_IEq1.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\rho \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ρ</mi> </math></EquationSource> </InlineEquation>-contraction<InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="44146_2025_208_Article_IEq15.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\}\)</EquationSource> <EquationSource Format="MATHML"><math> <mo stretchy="false">}</mo> </math></EquationSource> </InlineEquation>, (3) their similarity to contractions, (4) properties of their powers on a fixed vector, and (5) their unitary <InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="44146_2025_208_Article_IEq1.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\rho \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ρ</mi> </math></EquationSource> </InlineEquation>-dilations.</p>

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A brief survey on \(\rho \)-contractions and unitary \(\rho \)-dilations

  • Pei Yuan Wu,
  • Hwa-Long Gau

摘要

A bounded linear operator A on a complex Hilbert space H is a \(\rho \) ρ -contraction ( \(\rho >0\) ρ > 0 ) if there is a unitary operator U on space K containing H such that \(A^n=\rho P_HU^n|H\) A n = ρ P H U n | H for all \(n\ge 1\) n 1 , where \(P_H\) P H denotes the orthogonal projection from K onto H. U is called a unitary \(\rho \) ρ -dilation of A. Such operators originate from the early work of Sz.-Nagy and Foiaş (1966) and generalize the usual contractions and numerical contractions. In this survey, we briefly describe their properties, covering (1) their characterizations, (2) the related \(\rho \) ρ -radius, defined as \(w_{\rho }(A)=\inf \{\lambda >0 : (1/\lambda )A\) w ρ ( A ) = inf { λ > 0 : ( 1 / λ ) A is a \(\rho \) ρ -contraction \(\}\) } , (3) their similarity to contractions, (4) properties of their powers on a fixed vector, and (5) their unitary \(\rho \) ρ -dilations.